We performed the canonical transformation to eliminate the \(1/\varepsilon \)  pole terms in Ref. [1]}
before, where the corresponding terms have been given already. Here the multipole–moments have to be used in
\(D\)  dimensions, except for the last four terms in (REF ).
One obtains
\(H_{\rm tail, finite}^{\rm loc, 5PN} &=& \eta ^{10} \Biggl \lbrace H_{\rm el. quad}^{\rm 5PN}+ H_{\rm oct.}+ H_{\rm mag. quad.}+ H_{\rm ang.}+ H_{\rm mem. 1}+ H_{\rm mem. 2}+ H_{\rm mem. 3}\Biggr \rbrace .\) 
